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authorNao Pross <np@0hm.ch>2022-08-31 20:13:46 +0200
committerNao Pross <np@0hm.ch>2022-08-31 20:13:46 +0200
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kugel: Feedback and minor changes, add reference
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diff --git a/buch/papers/kugel/spherical-harmonics.tex b/buch/papers/kugel/spherical-harmonics.tex
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--- a/buch/papers/kugel/spherical-harmonics.tex
+++ b/buch/papers/kugel/spherical-harmonics.tex
@@ -871,8 +871,8 @@ computational cost lower by a factor of six \cite{davari_new_2013}.
The goal of this subsection's part is to apply the recurrence relations of the
$P^m_n(z)$ functions to the Spherical Harmonics. With some little adjustments
we will be able to have recursion equations for them too. As previously written
-the most of the work is already done. Now it is only a matter of minor
-mathematical operations/rearrangements. We can start by listing all of them:
+most of the work is already done. Now it is only a matter of minor mathematical
+operations/rearrangements. We can start by listing all of them:
\begin{subequations}
\begin{align}
Y^m_n(\vartheta, \varphi) &= \dfrac{1}{(2n+1)\cos \vartheta} \left[
@@ -899,7 +899,7 @@ mathematical operations/rearrangements. We can start by listing all of them:
\begin{proof}[Proof of \eqref{kugel:eqn:rec-sph-harm-1}]
We can multiply both sides of equality in \eqref{kugel:eqn:rec-leg-1} by $e^{im
\varphi}$ and perform the substitution $z=\cos \vartheta$. After a few simple
- algebraic steps, we will obtain the relation we are looking for
+ algebraic steps, we will obtain the relation we are looking for.
\end{proof}
\begin{proof}[Proof of \eqref{kugel:eqn:rec-sph-harm-2}]